/*===================================================================*/ /* NRDF D0357 Data No.10 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,10; D#=D357; TITLE=/APPLICATION OF THE CRYSTAL BLOCKING TECHNIQUE TO THE STUDY OF THE HIGHLY EXCITED NUCLEAR CONTINUUM/; PURPOSE=/TO EXAMINE CHANGES OF THE REACTION TIMES DUE TO ENHANCEMENT OF CERTAIN STATES AMONG THE MANY COMPOUND NUCLEAR FINE-STRUCTURE RESONANCES BY AN ISOBARIC ANALOGUE RESONANCE./; ATH=(W.M.GIBSON'1,2',M.MARUYAMA'3',Y.HASHIMOTO'3',E.P.KANTER'3', G.M.TEMMER'3',R.J.KEDDY'4',D.W.MINGAY'4',J.P.F.SELLSCHOP'4'); INST-ATH=(1USABEL'1',1USAALB'2',1USARUT'3',3SAFWIT'4'); /*@7@*/ REF=NP/A; VLP=317(1979)313; RCTS=(70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,10; ENR=NAT; CHM=ELN; THK-TGT=X'1'; /*@8@*/ BAC=C'2'; /*@11@*/ POL-TGT=NO; ACC=(VDG); INST-ACC=1USARUT; INC-ENGY-LAB-RANGE=(5.035MEV,5.110MEV,4.200MEV,3.708MEV,4.358MEV, 5.210MEV); POL-PRJ=NO; DET-PARTCL=(P); DET-SYS=(PS-SI); ERS-DET=58KEV; ANL=(DWBA,STATIST-MODEL,X'1'); /*@9@*/ PHQ=(X'1'); /*@14@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,10; INC-ENGY-LAB=5.110MEV; CMPD=73AS; RSD=72GE; /*FIG.7-(3)*/ /* D357 FIG.7-(3) */ /* SER#= 10 */ /* XSCALE=LINEAR YSCALE=LINEAR */ /* XMAX= 3.00000000E+04 YMAX= 9.99999642E-02 */ /* XMIN= 0.00000000E+00 YMIN= 0.00000000E+00 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'1' DELTA-DATA1 DATA2'2' DELTA-DATA2 (UCOULOMB) (UCOULOMB) (NODIM) (NODIM) 2788.595 1.034E+03 9.260E-02 1.793E-03 5397.289 1.574E+03 8.700E-02 2.242E-03 10434.770 1.529E+03 8.161E-02 1.793E-03 14842.566 7.196E+02 8.004E-02 2.242E-03 17001.488 7.646E+02 8.856E-02 1.793E-03 21364.309 1.529E+03 9.305E-02 1.793E-03 24737.621 8.545E+02 9.462E-02 1.793E-03 \END; /*===================================================================*/ |